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| DOE-HDBK-3010-94
7.0 Application Examples; Liquid Storage and Ion Exchange Examples
The RF assessed for this correlation is 0.3, which yields a combined ARF x RF of
5E-2. As this value is less than the combined ARF x RF of 7E-2 assessed for less
extreme conditions, the 7E-2 value is used. Therefore, this calculation winds up
estimating the same source term as the previous calculation that used the bounding
ARF x RF for less than 100 oC superheat.
7.3.6.3
Ion Exchange Example Assessment
The bounding initial respirable source term estimated for the example configuration (i.e.,
Pyrex columns) is 65 g of plutonium, although this value could be as low as 10 g or less
depending on when in the process the exotherm occurred and what percentage of resin
actually burned. However, definitively specifying such parameters is not possible. It is
probably best to estimate how much the source term would be reduced by the building
leakpath factor before expending effort trying to reduce the source term by arguments such
as the ability of fire suppression systems/practices or explosive dispersion to minimize the
amount of resin that actually burns. In any case, the appropriate focus is on identifying
controls to prevent and/or mitigate the accident. What is being determined by the source
term calculation is the level of priority of those controls, not an absolute assurance that a
release will be below a given value if preventive and mitigative systems fail.
Now that a spectrum of source terms has been developed, the potential nonconservatism of
assuming a thermal explosion as opposed to a chemical detonation can be revisited. If a
detonation had been assumed as the release model, burning resin release and flashing spray
would not be significant factors due to the speed of the reaction and its energy, which would
disperse resin widely. The guidance in this handbook would estimate that a mass of inert
material equal to the TNT equivalent mass of the detonation would go airborne. In the case
of the ion exchange column, the inert mass includes both resin and liquid in the resin bed.
The mass of resin in a column is ~ 15,000 g. The previous resin void volume estimate of
50% is reduced by half to 25% in order to minimize the mass of liquid. The resulting
estimate of 5.8 l of liquid would add an additional 5800 g of inert material if the density of
water is assumed. Therefore, any one ion exchange column would contain ~ 20,800 g of
inert material in the region where the explosion would take place. If total plutonium loading
is distributed between two columns, a maximum of 3250 g of plutonium would be in any one
column, resulting in an overall grams plutonium to grams inert ratio of 0.16.
The bounding release for the actual example was 65 g of plutonium. If an exotherm in one
column leads to an exotherm in the second loaded column, the explosion of each column
would have to generate 32.5 g of airborne plutonium. By the ratio just calculated, 203 g of
total material would go airborne to generate 32.5 g of airborne plutonium. This would
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